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In the title mol­ecule, C4H6N6O, the dihedral angle between the two triazole rings is 2.97 (1)°. The crystal structure is stabilized by one N—H...O, two O—H...N and three C—H...N(or O) hydrogen bonds, forming a three-dimensional network.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807020272/lh2370sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807020272/lh2370Isup2.hkl
Contains datablock I

CCDC reference: 647722

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](N-C) = 0.003 Å
  • R factor = 0.034
  • wR factor = 0.089
  • Data-to-parameter ratio = 6.6

checkCIF/PLATON results

No syntax errors found



Alert level A PLAT113_ALERT_2_A ADDSYM Suggests Possible Pseudo/New Spacegroup . C2/c
Author Response: Although the two triazole rings are related by pseudosymmetry. We can exclude centrosymmetric structure in space group of C2/c because (i) the R values are significantly worse (R1=15 and wR2=34%), (ii) the U values are more anisotropic than in Cc (iii) the structure is disordered.

Alert level B PLAT111_ALERT_2_B ADDSYM Detects (Pseudo) Centre of Symmetry ..... 100 PerFi
Alert level C PLAT089_ALERT_3_C Poor Data / Parameter Ratio (Zmax .LT. 18) ..... 6.61 PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 2 H2 O
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.00 From the CIF: _reflns_number_total 727 Count of symmetry unique reflns 729 Completeness (_total/calc) 99.73% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no
1 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Recent interest in substituted 1,2,4-triazoles has arisen in part from their transition metal complexes with intriguing structures and specific magnetic properties (Garcia et al.,1997; Kahn & Martinez,1998; Fujigaya et al.,2003). However bitriazole ligands have not been extensively exploited up to now, and herein we reported the crystal structure of (I).

In (I) (Fig.2), the two triazole ring are almost coplanar with a dihedral angle of 2.97 (1)° between them. The bond lengths and angles are unremarkable.

The crystal structure is stablized by one N–H···O, two O–H···N and three C–H···N(or O) hydrogen bonds. In detail, the water O atom O1 acts as a hydrogen bond donor, via. H1A and H1B, to the atom N5 at (-3/2 + x, 1/2 - y, -1/2 + z) and atom N6 (x, 1/2 + y, z), respectively, forming a one-dimensional chain along the [001] direction. In addition, the atom N2 at (x,y,z) acts as hydrogen bond donor, via. H2A, to the water O atom O1 in the same symmetric unit, linking adjacent chains into a three dimensional framework (Fig.3). Analysis using PLATON (Spek, 2003) shows that there are other three C–H···N(or O)(Table 2) hydrogen bonds which further stabilize the crystal structure. In addtion, ππ interactions are observed between the triazole ring N1—N3/C1/C2 at (x, y, z) and the other five-numbered ring N4—N6/C3/C4 at (-1 + x, y, z). The dihedral angle between the two triazole rings is only 2.97 (1)°, with an interplanar spacing of 3.273 (1) Å, a ring centroid separation of 3.635 (1) Å.

Related literature top

There has been recent interest in substituted 1,2,4-triazoles (Fujigaya et al., 2003; Garcia et al., 1997; Kahn & Martinez, 1998).

Experimental top

The title compound (I) was prepared by reacting diformylhydrazine (0.046 mol, 4.0 g) and 3-amino-1,2,4-triazole 0.046 mol,3.9 g). The reactant mixture was heated slowly to 433 K for an hour. The cooled reaction mixture was dissolved in 25 ml of boiling water and filtered. On cooling, 4.4 g of the product separated. Recrystallization from hot water gave large white crystals. Elemental analysis(%) for C4H6N6O, found (calculated): C 31.12 (31.13), H 3.80 (3.89), N 54.60 (54.49). IR(cm-1,KBr):3352.21, 3119.57,2881.59, 2733.65,1789.84,1657.08,1575.38,1505.81,1371.08,1303.73, 1290.26,1142.12, 1051.33,986.29, 958.04,897.31,877.09,738.58, 629.96,563.66.

Refinement top

When the structure of (I) is solved and refined in the centrosymmtric space group C2/c with half a molecule in the asymmetric unit, the structure is disordered with R values that are significantly higher (R1=15 and wR2=34%) and the anistropic displacement parameters have unusual values. In the absence of significant anomalous dispersion effects Friedel pairs were merged. H atoms bonded to O1 and N1 were located from the difference maps with and refined with constraints of O–H = 0.86 (2) Å, H–H =1.35 (2) Å, N–H = 0.86 (2) Å; Uiso(H) = 1.5Ueq(O) and Uiso(H) = 1.2Ueq(N). H2, H3 and H4 were placed in calculated positions with C—H = 0.93 Å and Uiso(H) =1.2Ueq(C).

Structure description top

Recent interest in substituted 1,2,4-triazoles has arisen in part from their transition metal complexes with intriguing structures and specific magnetic properties (Garcia et al.,1997; Kahn & Martinez,1998; Fujigaya et al.,2003). However bitriazole ligands have not been extensively exploited up to now, and herein we reported the crystal structure of (I).

In (I) (Fig.2), the two triazole ring are almost coplanar with a dihedral angle of 2.97 (1)° between them. The bond lengths and angles are unremarkable.

The crystal structure is stablized by one N–H···O, two O–H···N and three C–H···N(or O) hydrogen bonds. In detail, the water O atom O1 acts as a hydrogen bond donor, via. H1A and H1B, to the atom N5 at (-3/2 + x, 1/2 - y, -1/2 + z) and atom N6 (x, 1/2 + y, z), respectively, forming a one-dimensional chain along the [001] direction. In addition, the atom N2 at (x,y,z) acts as hydrogen bond donor, via. H2A, to the water O atom O1 in the same symmetric unit, linking adjacent chains into a three dimensional framework (Fig.3). Analysis using PLATON (Spek, 2003) shows that there are other three C–H···N(or O)(Table 2) hydrogen bonds which further stabilize the crystal structure. In addtion, ππ interactions are observed between the triazole ring N1—N3/C1/C2 at (x, y, z) and the other five-numbered ring N4—N6/C3/C4 at (-1 + x, y, z). The dihedral angle between the two triazole rings is only 2.97 (1)°, with an interplanar spacing of 3.273 (1) Å, a ring centroid separation of 3.635 (1) Å.

There has been recent interest in substituted 1,2,4-triazoles (Fujigaya et al., 2003; Garcia et al., 1997; Kahn & Martinez, 1998).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: PLATON.

Figures top
[Figure 1] Fig. 1. Reaction scheme.
[Figure 2] Fig. 2. Molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. The dashed line indicates an intermolecular hydrogen bond.
[Figure 3] Fig. 3. Part of the crystal structure of (I), showing the formation of a three-dimensional network from hydrogen bonding (dashed lines).
4-(1H-1,2,4-Triazol-3-yl)-4H-1,2,4-triazole monohydrate top
Crystal data top
C4H4N6·H2OF(000) = 320
Mr = 154.15Dx = 1.538 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2ycCell parameters from 1837 reflections
a = 3.8716 (3) Åθ = 2.6–28.1°
b = 15.8019 (14) ŵ = 0.12 mm1
c = 10.8874 (9) ÅT = 296 K
β = 91.785 (1)°Plate, colorless
V = 665.75 (10) Å30.20 × 0.10 × 0.04 mm
Z = 4
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
727 independent reflections
Radiation source: fine focus sealed Siemens Mo tube709 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
0.3° wide ω exposures scansθmax = 27.0°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
h = 44
Tmin = 0.976, Tmax = 0.988k = 1820
2254 measured reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.089H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0579P)2 + 0.1815P]
where P = (Fo2 + 2Fc2)/3
727 reflections(Δ/σ)max < 0.001
110 parametersΔρmax = 0.17 e Å3
6 restraintsΔρmin = 0.21 e Å3
Crystal data top
C4H4N6·H2OV = 665.75 (10) Å3
Mr = 154.15Z = 4
Monoclinic, CcMo Kα radiation
a = 3.8716 (3) ŵ = 0.12 mm1
b = 15.8019 (14) ÅT = 296 K
c = 10.8874 (9) Å0.20 × 0.10 × 0.04 mm
β = 91.785 (1)°
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
727 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
709 reflections with I > 2σ(I)
Tmin = 0.976, Tmax = 0.988Rint = 0.027
2254 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0346 restraints
wR(F2) = 0.089H atoms treated by a mixture of independent and constrained refinement
S = 1.06Δρmax = 0.17 e Å3
727 reflectionsΔρmin = 0.21 e Å3
110 parameters
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.1950 (6)0.28332 (13)0.7395 (2)0.0286 (5)
C20.0527 (8)0.39041 (17)0.7999 (2)0.0403 (6)
H20.14310.43310.84810.048*
C30.4923 (7)0.16139 (17)0.6439 (2)0.0383 (6)
H30.44330.17450.56190.046*
C40.5157 (8)0.16590 (16)0.8413 (2)0.0363 (6)
H40.48670.18290.92220.044*
N10.0761 (6)0.31653 (13)0.63646 (19)0.0363 (5)
N20.0840 (6)0.38719 (14)0.67866 (19)0.0378 (5)
H2A0.187 (8)0.4237 (18)0.627 (3)0.052 (9)*
N30.1248 (7)0.32463 (13)0.84350 (19)0.0385 (6)
N40.3879 (5)0.20801 (11)0.74086 (18)0.0293 (4)
N50.6829 (6)0.09913 (14)0.80910 (18)0.0406 (6)
N60.6694 (7)0.09619 (14)0.6813 (2)0.0412 (5)
O10.4451 (6)0.48966 (11)0.5130 (2)0.0423 (5)
H1A0.584 (9)0.465 (2)0.466 (3)0.064*
H1B0.561 (9)0.5245 (19)0.553 (3)0.064*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0330 (12)0.0295 (9)0.0236 (9)0.0055 (8)0.0036 (8)0.0001 (8)
C20.0498 (16)0.0358 (12)0.0356 (13)0.0012 (10)0.0075 (11)0.0059 (10)
C30.0481 (16)0.0390 (12)0.0278 (11)0.0028 (10)0.0025 (11)0.0035 (9)
C40.0460 (14)0.0405 (12)0.0224 (10)0.0007 (10)0.0013 (10)0.0025 (9)
N10.0455 (13)0.0365 (11)0.0268 (9)0.0037 (8)0.0011 (8)0.0003 (7)
N20.0440 (13)0.0332 (10)0.0363 (10)0.0019 (8)0.0039 (9)0.0028 (8)
N30.0513 (14)0.0393 (11)0.0251 (9)0.0028 (9)0.0041 (9)0.0040 (7)
N40.0346 (11)0.0325 (9)0.0208 (7)0.0021 (7)0.0011 (7)0.0002 (7)
N50.0477 (15)0.0401 (12)0.0336 (11)0.0011 (9)0.0034 (9)0.0049 (8)
N60.0472 (14)0.0390 (12)0.0373 (11)0.0036 (10)0.0030 (10)0.0022 (9)
O10.0460 (10)0.0415 (10)0.0393 (11)0.0033 (9)0.0030 (8)0.0040 (7)
Geometric parameters (Å, º) top
C1—N11.309 (3)C4—N51.292 (4)
C1—N31.342 (3)C4—N41.360 (3)
C1—N41.405 (3)C4—H40.9300
C2—N21.323 (3)N1—N21.364 (3)
C2—N31.326 (4)N2—O12.770 (3)
C2—H20.9300N2—H2A0.895 (18)
C3—N61.296 (4)N5—N61.392 (3)
C3—N41.359 (3)O1—H1A0.835 (18)
C3—H30.9300O1—H1B0.840 (19)
N1—C1—N3116.9 (2)C2—N2—O1131.0 (2)
N1—C1—N4121.40 (19)N1—N2—O1119.00 (16)
N3—C1—N4121.67 (19)C2—N2—H2A129 (2)
N2—C2—N3111.0 (3)N1—N2—H2A121 (2)
N2—C2—H2124.5C2—N3—C1101.3 (2)
N3—C2—H2124.5C3—N4—C4104.5 (2)
N6—C3—N4110.7 (2)C3—N4—C1128.46 (19)
N6—C3—H3124.6C4—N4—C1127.06 (19)
N4—C3—H3124.6C4—N5—N6107.2 (2)
N5—C4—N4110.7 (2)C3—N6—N5106.9 (2)
N5—C4—H4124.6N2—O1—H1A115 (3)
N4—C4—H4124.6N2—O1—H1B108 (3)
C1—N1—N2101.0 (2)H1A—O1—H1B107 (3)
C2—N2—N1109.8 (2)
N3—C1—N1—N20.8 (3)N6—C3—N4—C1179.3 (2)
N4—C1—N1—N2179.09 (19)N5—C4—N4—C30.2 (3)
N3—C2—N2—N10.3 (3)N5—C4—N4—C1179.5 (2)
N3—C2—N2—O1175.2 (2)N1—C1—N4—C33.1 (3)
C1—N1—N2—C20.6 (3)N3—C1—N4—C3176.8 (3)
C1—N1—N2—O1176.24 (17)N1—C1—N4—C4177.7 (3)
N2—C2—N3—C10.2 (3)N3—C1—N4—C42.4 (3)
N1—C1—N3—C20.6 (3)N4—C4—N5—N60.3 (3)
N4—C1—N3—C2179.2 (2)N4—C3—N6—N50.2 (3)
N6—C3—N4—C40.0 (3)C4—N5—N6—C30.4 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1A···N5i0.84 (2)2.15 (2)2.962 (3)163 (4)
O1—H1B···N6ii0.84 (2)2.10 (2)2.930 (3)169 (4)
C2—H2···O1iii0.932.493.392 (3)163
C3—H3···N3iv0.932.503.334 (3)149
C4—H4···N1v0.932.353.226 (3)157
N2—H2A···O10.90 (2)1.88 (2)2.770 (3)173 (3)
Symmetry codes: (i) x3/2, y+1/2, z1/2; (ii) x3/2, y+1/2, z; (iii) x, y+1, z+1/2; (iv) x+1/2, y+1/2, z1/2; (v) x+1/2, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC4H4N6·H2O
Mr154.15
Crystal system, space groupMonoclinic, Cc
Temperature (K)296
a, b, c (Å)3.8716 (3), 15.8019 (14), 10.8874 (9)
β (°) 91.785 (1)
V3)665.75 (10)
Z4
Radiation typeMo Kα
µ (mm1)0.12
Crystal size (mm)0.20 × 0.10 × 0.04
Data collection
DiffractometerBruker SMART APEX CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 2001)
Tmin, Tmax0.976, 0.988
No. of measured, independent and
observed [I > 2σ(I)] reflections
2254, 727, 709
Rint0.027
(sin θ/λ)max1)0.639
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.034, 0.089, 1.06
No. of reflections727
No. of parameters110
No. of restraints6
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.17, 0.21

Computer programs: SMART (Bruker, 2001), SAINT-Plus (Bruker, 2001), SAINT-Plus, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), PLATON.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1A···N5i0.835 (18)2.15 (2)2.962 (3)163 (4)
O1—H1B···N6ii0.840 (19)2.10 (2)2.930 (3)169 (4)
C2—H2···O1iii0.932.493.392 (3)162.8
C3—H3···N3iv0.932.503.334 (3)149.2
C4—H4···N1v0.932.353.226 (3)157.4
N2—H2A···O10.895 (18)1.879 (19)2.770 (3)173 (3)
Symmetry codes: (i) x3/2, y+1/2, z1/2; (ii) x3/2, y+1/2, z; (iii) x, y+1, z+1/2; (iv) x+1/2, y+1/2, z1/2; (v) x+1/2, y+1/2, z+1/2.
 

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